Quasistationarity in a long-range interacting model of particles moving on a sphere
arXiv:1309.0194 · doi:10.1103/PhysRevE.88.052137
Abstract
We consider a long-range interacting system of particles moving on a spherical surface under an attractive Heisenberg-like interaction of infinite range, and evolving under deterministic Hamilton dynamics. The system may also be viewed as one of globally coupled Heisenberg spins. In equilibrium, the system has a continuous phase transition from a low-energy magnetized phase, in which the particles are clustered on the spherical surface, to a high-energy homogeneous phase. The dynamical behavior of the model is studied analytically by analyzing the Vlasov equation for the evolution of the single-particle distribution, and numerically by direct simulations. The model is found to exhibit long lived non-magnetized quasistationary states (QSSs) which in the thermodynamic limit are dynamically stable within an energy range where the equilibrium state is magnetized. For finite , these states relax to equilibrium over a time that increases algebraically with . In the dynamically unstable regime, non-magnetized states relax fast to equilibrium over a time that scales as . These features are retained in presence of a global anisotropy in the magnetization.
9 pages, 4 figures; v2: refs. added, published version
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